1. Status of the CLIC main beam injectors LCWS, Arlington, Texas, October 22 th -26 th, 2012Steffen Döbert, BE-RF Overview of the CLIC main beam injectors complex as documented in the CDR

2. Layout Primary 5 GeV e - Linac Injector Linac Booster Linac 2 GHz Pre-injector e + Linac Pre-injector e - Linac e - DR gun PDR e + DR DL’s BC1 DC gun target 9 GeV 2.86 GeV 0.2 GeV PDR Spin rotatator Two hybrid positron sources (only one needed for 3 TeV) Common injector linac All linac at 2 GHz, bunch spacing 1 GHz before the damping rings

3. Zoom e - transfer line e + transfer line e - and e + sources e - and e + Damping Rings CLIC Main Beam complex

4. Beam timing and operational modes Before damping ring (1 GHz bunch spacing) e-e- e+e+ e+e+ e-e- 2314 ns 717 ns 156-556 ns After damping ring (2 GHz bunch spacing) e-e- e+e+ 1100 ns 156-556 ns Operational mode Charge per bunch (nC) Number of bunches Nominal0.6312 500 GeV1.2312 Low energy scans 0.6, 0.45, 0.4, 0.3, 0.23312, 472, 552, 792, 1112

5. Beam parameters ParameterUnit CLIC polarized electrons CLIC positrons CLIC booster EGeV2.86 9 N10 9 4.3 3.75 nbnb -312 tbtb ns11 0.5 t pulse ns312 156  x,y mm < 1007071, 7577 600,10 ∙10 -3 zz mm< 43.3 44 ∙10 -3 EE %< 11.63 1.7 Charge stability shot-to-shot %0.1 Charge stability flatness on flat top %0.1 f rep Hz50 PkW29 85

6. Polarized electron source DC-gun, 140 kV GaAs cathode 1 GHz buncher2 GHz buncher + accelerator Polarized laser Classical polarized source wit bunching system Charge production demonstrated by SLAC experiment Simulations showed 87 % capture efficiency (F. Zou, SLAC)

7. Polarized electron source parameters POLARIZED SOURCE FOR CLIC Electrons CLIC 1 GHz CLIC DC/ SLAC Demo Number of electrons per bunch (*10^9)3.721365 Charge/single bunch (nC)0.96NA Charge/macrobunch (nC)300 Bunch spacing(ns)1DC RF frequeny (GHz)1DC Bunch length at cathode (ps)100DC Number of bunches312NA Repetition rate (Hz)50 QE(%)0.3 Polarization >80% Circular polarization >99% Laser wavelength (nm) Laser 780-880865 Energy/micropulse on cathode (nJ)509NA Energy/macropulse on cathode (μJ)159190 Energy/micropulse laser room (nJ)1526NA Energy/macrop. Laser room (μJ)476633 Mean power per pulse (kW)1.52 Average power at cathode wavelength(mW)89.5 Laser scheme For the 1 GHz approach cathode current densities of 3-6 A/cm 2 would be needed, the dc approach uses < 1 A/cm 2

8. Polarized electron source CLIC Goal 0.5 TeV: 35e11 J. Shepard

9. Positron source conventional ? Primary beam Linac for e - 2 GHz AMD Gun 5 GeV Primary beam Linac for e - 200 MeV Hybrid target AMD Primary beam Linac for e - 200 MeV Hybrid target RF- deflector Bunch compressor AMD: 200 mm long, 20 mm radius, 6T field

10. Hybrid target Target Parameters Crystal MaterialTungstenW Thickness (radiation length)0.4  Thickness (length)1.40mm Energy deposited~1kW Target Parameters Amorphous MaterialTungstenW Thickness (Radiation length)3  Thickness (length)10mm PEDD30J/g Distance to the crystal2m

11. Primary electron beam and linac Parameters Energy5GeV Number of e - / bunch1.1x10 10 Charge / bunch1.8nC Bunches per pulse312 Pulse repetition rate50Hz Beam radius (rms)2.5mm Bunch length (rms)1ps Beam power140kW Can be done with thermionic gun or photo injector (CTF3 and Phin are nice references) 2 GHz rf system as used for other injector linac’s

12. Yield simulations capture and pre-injector linac Accelerating modedecelerating mode Energy density at 200 MeV O. Dadoun Positron yield: after target: ~8 e + /e - at 200 MeV: 0.9 e + /e - into PDR: 0.39 e + /e -

13. Common injector linac

14. Injector linac rf system Structure ParameterValue Frequency1998 MHz Structure length (30 cells)1.5 m Filling time389 ns Cell length and iris thickness50 mm, 8 mm Shunt impedance 54.3 – 43.3 M  /m Aperture a20 – 14 mm Cell size b64.3 – 62.9 Group velocity vg/c2.54 -0.7 % Phase advance per cell2  /3 Acc 1Acc 2Acc 3Acc 4 Quad BPM ModPulse compressor Kly 1 Kly 2 50 MW, 8  s 250 MW, 1.5  s

15. Linac structure beam loading and power flow Parameters: tapered f= 1998 MHz L= 1.5 m Pin= 53.4 MW Nb= 312 N = 4.0 e9 Eacc = 16 MV/m Eff = 16.5% Almost full loading for 500 GeV parameters, will need amplitude modulation for beam loading compensation

16. Bunch compressors Two stages of bunch compressors, CSR, wake fields and tolerances have been studied BC1, 2.86 GeVBC2, 9 GeV Rf frequency2 GHz, 15 MV/m12 GHz, 74 MV/m Phase tolerance0.1 deg Bunch length after compression 300  m factor 5.3 44  m factor 6.8 Enegy spread after compression 0.25 %1.7 % Voltage447 MV1776 MV

17. Linac Parameters Primary 5 GeV e - Linac Injector Linac Booster Linac 2 GHz Pre-injector e + Linac Pre-injector e - Linac e - DR gun PDR e + DR DL’s BC1 DC gun target 9 GeV 2.86 GeV 0.2 GeV PDR Spin rotatator

18. CDR, what’s next ?  Start work on low energy machine  Cost optimization, Pre-damping ring, positron driver linac  Follow up some issues from the CDR within the CLIC work package structure  More focus on polarized positron studies in the future, revisit undulator scheme, study polarization transport

19. Potential for cost reduction Cut pre-damping ring for electrons: Which transverse and longitudinal emittance is needed from 200 MeV linac ? Emittance possible: 25 - 50  m, do we need more energy ? Reduce beam power of positron drive linac: Lower beam current and use multiple injection into PDR, timing ? Lower beam energy (less yield) and use multiple injection Saving potential ? Use booster linac as well as positron drive linac: Save entire linac +tunnel (>160 MCHF), need more rf power in booster linac, Put injector linac in same tunnel as booster (see layout)

20. Alternative layout Without positron driver linac Injector Linac Booster Linac 2 GHz Pre-injector e - Linac e - DR gun PDR e + DR DL’s BC1 DC gun target 6 GeV 2.86 GeV 0.2 GeV PDR e-e- e-e- 3300 ns 156ns e+e+ Positron production pulse

21. Pre-Damping ring acceptance

22. Omori’s ERL scheme for CLIC

26. Compton-ring for CLIC

28. Compton Ring Parameters: E=1 GeV, 2 GHz, 312 bunches, 6.2 10 10 e - /bunch, 156 ns Circumference 60% polarization Laser Energy 590 mJ Yield: 2.1 10 9 photons/turn/bunch 10 7 e +.turn/bunch  440 turn stacking in Pre-damping ring to get 4.2 10 9 positrons Compton Linac option: 10 laser IP’s, 4 GeV linac with 5 nC/bunch, (could we use the drive beam linac) How realistic are 10 laser IP’s ?

29. CLIC Compton schemes for polarized positron production  Not much done since 2010, ring scheme by Eugene et al., ERL scheme by Omori-san, Linac scheme studied as well  Stacking needed either in PDR or dedicated rings  Compton-ring was considered most promising  Difficult to judge how realistic the schemes are Any comments ?  How about direct conversion from polarized electrons as done by JLAB ? Any feelings ? Conversion yield ~10 -3, 1000 x times stacking ? What would be optimized parameters

30. Conclusions  Big effort to get the conceptual design of the CLIC main beam injectors, rather conceptual in many places but main problems studied and identified  General believe that the injectors are feasible and relatively conservative approaches are used  Obviously more work remains to be done

31. Collaborations Polarized electron source:SLAC, TJNAF Positron source: KEK, LAL Polarized positrons: KEK, LAL, ANL, CI, KIPT, Ankara University

32. Linac Parameters and cost Primary 5 GeV e - Linac Injector Linac Booster Linac 2 GHz Pre-injector e + Linac Pre-injector e - Linac e - DR gun PDR e + DR DL’s BC1 DC gun target 9 GeV 2.86 GeV 0.2 GeV PDR Spin rotatator

33. Linac structure beam loading and power flow Parameters: tapered f= 1998 MHz L= 3 m Pin= 77 MW Nb= 624 N = 4.0 e9 Eacc = 15 MV/m